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Diffstat (limited to 'tests/rayleigh.py')
-rw-r--r-- | tests/rayleigh.py | 56 |
1 files changed, 56 insertions, 0 deletions
diff --git a/tests/rayleigh.py b/tests/rayleigh.py new file mode 100644 index 0000000..4394ada --- /dev/null +++ b/tests/rayleigh.py @@ -0,0 +1,56 @@ +import unittest +import numpy as np + +from chroma.geometry import Solid, Geometry +from chroma.make import box +from chroma.sim import Simulation +from chroma.optics import water_wcsim +from chroma.event import Photons +import histogram +from histogram.root import rootify +import ROOT +ROOT.gROOT.SetBatch(1) + +class TestRayleigh(unittest.TestCase): + def setUp(self): + self.cube = Geometry() + self.cube.add_solid(Solid(box(100,100,100), water_wcsim, water_wcsim)) + self.cube.pmtids = [0] + self.sim = Simulation(self.cube, water_wcsim, bvh_bits=4, geant4_processes=0, + use_cache=False) + nphotons = 100000 + positions = np.tile([0,0,0], (nphotons,1)).astype(np.float32) + directions = np.tile([0,0,1], (nphotons,1)).astype(np.float32) + polarizations = np.zeros_like(positions) + phi = np.random.uniform(0, 2*np.pi, nphotons).astype(np.float32) + polarizations[:,0] = np.cos(phi) + polarizations[:,1] = np.sin(phi) + times = np.zeros(nphotons, dtype=np.float32) + wavelengths = np.empty(nphotons, np.float32) + wavelengths.fill(400.0) + + self.photons = Photons(positions=positions, directions=directions, polarizations=polarizations, + times=times, wavelengths=wavelengths) + + def testAngularDistributionPolarized(self): + # Fully polarized photons + self.photons.polarizations[:] = [1.0, 0.0, 0.0] + + photon_stop = self.sim.propagate_photons(self.photons, max_steps=1) + aborted = (photon_stop.histories & (1 << 31)) > 0 + self.assertFalse(aborted.any()) + + # Compute the dot product between initial and final directions + rayleigh_scatters = (photon_stop.histories & (1 << 4)) > 0 + cos_scatter = (self.photons.directions[rayleigh_scatters] * photon_stop.directions[rayleigh_scatters]).sum(axis=1) + theta_scatter = np.arccos(cos_scatter) + h = histogram.Histogram(bins=100, range=(0, np.pi)) + h.fill(theta_scatter) + h = rootify(h) + + # The functional form for polarized light should be (1 + \cos^2 \theta)\sin \theta + # according to GEANT4 physics reference manual + f = ROOT.TF1("pol_func", "[0]*(1+cos(x)**2)*sin(x)", 0, np.pi) + h.Fit(f) + self.assertGreater(f.GetProb(), 1e-3) + |